\begin{table}%t3
\par
\caption {\label{tab:lines}List of strongest \ion{Fe}{viii} lines in the 100--500~\AA\ range. 
}
%\centerline
 {\tiny 
\begin{tabular}[c]{@{}ccccrlllll@{}}
\hline \hline  
\noalign{\smallskip}
 $i-j$ & Levels   &  Int & $gf$ & G00 & Z03 D &  $A_{ji}$(s$^{-1}$) &   $\lambda_{\rm exp}$(\AA) & $\lambda_{\rm th}$(\AA)   & ID \\  
\hline                                   %inserts single line
2--49 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$D$_{5/2}$ & 1.0 & 7.06 & 9.1 & 7.2 & $2.8 \times 10^{11}$ & 168.173 & 159.73 &    G65 \\ 
2--46 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{7/2}$ & 0.90 & 3.92 & 5.8 & 4.2 & 
$9.5 \times  10^{10}$ & 185.213 & 178.09 &    G65 \\ 
1--50 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$D$_{3/2}$ & 0.58 & 4.56 & 5.9 & 4.6 & 
$2.7 \times 10^{11}$ & 167.486 & 159.20 &    G65 \\ 
2--48 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$P$_{3/2}$ & 0.57 & 3.82 & 4.3 & 3.7 & 
$2.2 \times  10^{11}$ & 168.544 & 162.16 &    RR80 \\ 
1--45 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & 0.58 & 2.80 & 4.1 & 2.9 & 
$9.0 \times  10^{10}$ & 186.599 & 179.25 &    G65 \\ 
1--47 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$P$_{1/2}$ & 0.29 & 2.10 & 2.4 & 2.0 & 
$2.4 \times  10^{11}$ & 168.929 & 162.43 &    RR80 \\ 
2--43 & 3p$^6$3d $^2$D$_{5/2}$--3p$^6$4p $^2$P$_{3/2}$ & 0.29 & 0.67 & 0.60 & --  & 
$3.0 \times  10^{10}$ & 194.661 & 191.39 &    RR80 \\ 
2--54 & 3p$^6$3d $^2$D$_{5/2}$--3p$^6$4f $^2$F$_{7/2}$ & 0.14 & 4.30 & 4.0 & --  & 
$2.1 \times  10^{11}$ & 131.240 & 129.02 &    KW37 \\ 
1--42 & 3p$^6$3d $^2$D$_{3/2}$--3p$^6$4p $^2$P$_{1/2}$ & 0.17 & 0.38 & 0.38 & --  & 
$3.3 \times 10^{10}$ & 195.972 & 192.88 &    ? RR80 \\ 
1--53 & 3p$^6$3d $^2$D$_{3/2}$--3p$^6$4f $^2$F$_{5/2}$ & $9.0\times  10^{-2}$ & 2.97 & 2.8 & --  & $1.9 \times 10^{11}$ & 130.941 & 128.71 &    KW37 \\ 
2--26 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{7/2}$ & 0.14 & 0.14 & 0.10 & --  & 
$2.2 \times 10^{9}$ & 224.305 & 223.88 &    RR80 \\ 
2--6 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$D$_{7/2}$ & 0.15 & $2.1\times  10^{-4}$ & 
$2.2 \times 10^{-4}$ & --  & $2.8 \times 10^{6}$ & 253.956 & 257.79 &    N \\ 
2--22 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{7/2}$ & 0.12 & 
$5.6\times 10^{-2}$ & $5.2 \times 10^{-2}$ & --  & 
$8.8 \times 10^{8}$ & 231.097 & 231.15 &    RR80 \\ 
2--9 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$G$_{7/2}$ & $9.9 \times 10^{-2}$ & 
$1.0 \times 10^{-4}$ & $7.0 \times 10^{-5}$ & --  & $1.4\times  10^{6}$ &  --  & 243.92 &   \\ 
2--17 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$F$_{7/2}$ & 
$9.5 \times 10^{-2}$ & $8.1 \times 10^{-4}$ & 
$4.8 \times 10^{-4}$ & --  & $1.2 \times 10^{7}$ &  --  & 235.41 &   \\ 
2--21 & 3p$^6$3d $^2$D$_{5/2}$--3p$^6$4s $^2$S$_{1/2}$ & $8.9 \times 10^{-2}$ & -- & 0.0 & --  & 
$6.5 \times 10^{5}$ & --  & 231.69 &   \\ 
1--30 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & $8.1\times  10^{-2}$ & 0.12 & 0.10 & --  & $2.9\times 10^{9}$ & 217.691 & 217.17 &    RR80 \\ 
1--49 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$D$_{5/2}$ & $6.1 \times 10^{-2}$ & 0.43 & 0.57 & 0.51 & $1.7\times  10^{10}$ & 167.655 & 159.24 &    G65 \\ 
2--50 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$D$_{3/2}$ & $5.6 \times 10^{-2}$ & 0.44 & 0.64 & 0.51 & $2.6 \times 10^{10}$ & 168.003 & 159.69 &    G65 \\ 
1--48 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$P$_{3/2}$ & $5.5 \times 10^{-2}$ & 0.37 & 0.48 & 0.41 & $2.2 \times 10^{10}$ & 168.024 & 161.65 &    RR80 \\ 
2--5 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$D$_{5/2}$ & $8.3 \times 10^{-2}$ & $2.4 \times 10^{-4}$ & $2.2\times  10^{-4}$ & --  & $4.0\times 10^{6}$ & 255.350 & 259.31 &    N \\ 
2-24 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$P$_{3/2}$ & $7.3 \times 10^{-2}$ & $2.2 \times 10^{-2}$ & $1.6\times 10^{-2}$ & $2.1 \times 10^{-2}$ & $7.2 \times 10^{8}$ & 225.396 & 225.29 &    N \\ 
2-31 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$D$_{7/2}$ & $7.0 \times 10^{-2}$ & $1.3\times 10^{-4}$ & $1.1 \times 10^{-4}$ & --  & $2.2 \times 10^{6}$ &  -- & 217.51 &   \\ 
2--16 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$F$_{9/2}$ & $7.2\times 10^{-2}$ & $4.5 \times 10^{-12}$ & 0.0 & --  & 45. &  --  & 235.87 &   \\ 
1--19 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & $6.7\times 10^{-2}$ & $4.1\times 10^{-2}$ & $3.2 \times 10^{-2}$ & --  & $8.5 \times 10^{8}$ & 231.884 & 232.05 &    RR80 \\ 
2--18 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$D$_{5/2}$ & $6.7\times 10^{-2}$ & 
$8.8\times 10^{-4}$ & $1.6 \times 10^{-6}$ & --  & $1.8\times 10^{7}$ &  --  & 233.49 &   \\ 
2--27 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$G$_{7/2}$ & $6.3 \times 10^{-2}$ & $1.1 \times 10^{-2}$ & $3.6 \times 10^{-2}$ & --  & $1.8\times  10^{8}$ & 222.190 & 222.57 &    N \\ 
2--41 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$P$_{3/2}$ & $5.2\times 10^{-2}$ & 
$9.9 \times 10^{-2}$ & 0.19 & 0.13 & $4.3 \times 10^{9}$ & 197.362 & 194.03 &    RR80 \\ 
1--21 & 3p$^6$3d $^2$D$_{3/2}$--3p$^6$4s $^2$S$_{1/2}$ & $5.9 \times 10^{-2}$ & -- & 0.0 & --  & $4.3 \times 10^{5}$ &  --  & 230.66 &   \\ 
1--36 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$D$_{5/2}$ & $5.3 \times 10^{-2}$ & 
$3.7 \times 10^{-3}$ & $2.2 \times 10^{-3}$ & --  & $9.5\times 10^{7}$ & 207.124 & 205.01 &    N \\ 
2--10 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$P$_{5/2}$ & $5.9 \times 10^{-2}$ & 
$1.3 \times 10^{-4}$ & $1.0\times 10^{-4}$ & --  & $2.5\times 10^{6}$ &  --  & 243.30 &   \\ 
1--4 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$D$_{3/2}$ & $5.1\times 10^{-2}$ & 
$1.1\times 10^{-4}$ & $1.1\times 10^{-4}$ & --  & $2.8\times 10^{6}$ & 255.110 & 259.05 &    N \\ 
2--20 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$D$_{3/2}$ & $4.5 \times 10^{-2}$ & 
$6.0\times 10^{-3}$ & $3.3\times 10^{-3}$ & --  & $1.9\times 10^{8}$ &  --  & 232.52 &   \\ 
2--40 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$G$_{7/2}$ & $3.9 \times  10^{-2}$ & 
$2.2\times 10^{-2}$ & $1.8\times 10^{-2}$ & --  & $4.3\times 10^{8}$ & 204.704 & 203.12 &    N \\ 
1--15 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$F$_{5/2}$ & $4.2\times 10^{-2}$ & $5.8\times 10^{-3}$ & $3.9\times 10^{-3}$ & --  & $1.2\times 10^{8}$ &  --  & 235.12 &   \\ 
2--32 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$D$_{5/2}$ & $3.5\times 10^{-2}$ & $2.8 \times10^{-3}$ & $1.6\times 10^{-3}$ & --  & $6.5\times 10^{7}$ &  --  & 216.87 &   \\ 
1--14 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$F$_{3/2}$ & $3.8\times  10^{-2}$ & $5.7\times 10^{-3}$ & $4.9 \times 10^{-3}$ & --  & $1.7 \times 10^{8}$ &  --  & 235.83 &   \\ 
1--43 & 3p$^6$3d $^2$D$_{3/2}$--3p$^6$4p $^2$P$_{3/2}$ & $3.1 \times 10^{-2}$ & $7.1\times  10^{-2}$ & $6.1\times 10^{-2}$ & --  & $3.2 \times 10^{9}$ & 193.968 & 190.69 &    RR80 \\ 
1--23 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$P$_{1/2}$ & $3.4\times  10^{-2}$ & $1.5\times  10^{-2}$ & $1.0 \times  10^{-2}$ & --  & $9.4\times  10^{8}$ & 227.290 & 227.10 &    N \\ 
2--45 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & $2.5 \times 10^{-2}$ & 0.12 & 0.21 & 0.20 & $3.9\times  10^{9}$ & 187.240 & 179.87 &    RR80 \\ 
1--35 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$D$_{3/2}$ & $2.2 \times 10^{-2}$ & $2.6\times 10^{-3}$ & $1.9\times 10^{-3}$ & --  & $9.8\times  10^{7}$ &  --  & 206.68 &   \\ 
2--11 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$G$_{5/2}$ & $2.4\times 10^{-2}$ & 
$5.5\times 10^{-5}$ & $6.2\times 10^{-5}$ & --  & 
$1.1\times 10^{6}$ &  --  & 242.64 &   \\ 
1--3 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$D$_{1/2}$ & $2.5\times 10^{-2}$ & 
$1.6\times 10^{-5}$ & $1.8\times 10^{-5}$ & --  & $8.0\times 10^{5}$ & 255.684 & 259.66 &    N \\ 
1--44 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$P$_{1/2}$ & $1.6\times 10^{-2}$ & $4.0\times 10^{-2}$ & $5.9\times 10^{-2}$ & $6.0\times 10^{-2}$ & $3.6\times 10^{9}$ & 192.004 & 188.74 &    ? RR80 \\ 
2--12 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$P$_{3/2}$ & $1.9\times 10^{-2}$ & 
$7.6\times 10^{-5}$ & $1.2\times 10^{-4}$ & --  & $2.2\times  10^{6}$ &  -- & 241.53 &   \\ 
2--25 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$H$_{11/2}$ & $1.6 10^{-2}$ & 
$1.0\times  10^{-10}$ & 0.0 & --  & 1.1 &  --  & 224.95 &   \\ 
2--33 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$D$_{3/2}$ & $1.6 \times 10^{-2}$ & $2.9\times  10^{-3}$ & $2.3 \times 10^{-3}$ & --  & $1.0 \times 10^{8}$ &  --  & 215.96 &   \\ 
2--15 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$F$_{5/2}$ & $1.6 \times 10^{-2}$ & $2.3\times  10^{-3}$ & $2.6\times 10^{-3}$ & --  & $4.6\times 10^{7}$ &  --  & 236.19 &   \\ 
2--28 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$G$_{9/2}$ & $1.5 \times 10^{-2}$ & $8.2 \times 10^{-11}$ & 0.0 & --  & 9.7 &  --  & 221.16 &   \\ 
2--37 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$S$_{3/2}$ & $1.3 \times 10^{-2}$ & $7.9 \times 10^{-3}$ & $6.2 \times 10^{-3}$ & --  & $3.1\times 10^{8}$ & 207.124 & 204.74 &   \\ 
2--30 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & $1.3 \times 10^{-2}$ & $2.0 \times 10^{-2}$ & $1.8\times 10^{-2}$ & --  & $4.7\times 10^{8}$ & 218.564 & 218.09 &    RR80 \\ 
1--10 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$P$_{5/2}$ & $1.4 \times 10^{-2}$ & $3.1 \times 10^{-5}$ & $2.7\times 10^{-5}$ & --  & $6.0 \times 10^{5}$ &  --  & 242.16 &   \\ 
1--13 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$P$_{1/2}$ & $1.4 \times 10^{-2}$ & $1.5 \times 10^{-5}$ & $2.5 \times 10^{-5}$ & --  & $8.7 \times 10^{5}$ &  --  & 239.13 &   \\ 
2--53 & 3p$^6$3d $^2$D$_{5/2}$--3p$^6$4f $^2$F$_{5/2}$ & $6.5\times  10^{-3}$ & 0.22 & 0.20 & --  & $1.4 \times 10^{10}$ & 131.257 & 129.03 &    RR80 \\ 
1--12 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$P$_{3/2}$ & $1.2\times  10^{-2}$ & $4.8 \times 10^{-5}$ & $5.1\times 10^{-5}$ & --  & $1.4\times 10^{6}$ &  --  & 240.40 &   \\ 
1--41 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^2$P$_{3/2}$ & $9.6 \times 10^{-3}$ & $1.8 \times 10^{-2}$ & $2.8\times 10^{-2}$ & $1.5 \times 10^{-2}$ & $7.8\times  10^{8}$ & 196.650 & 193.30 &    RR80 \\ 
2--35 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$D$_{3/2}$ & $8.7 \times 10^{-3}$ & $1.0 \times 10^{-3}$ & $6.8\times 10^{-4}$ & --  & $4.0 \times 10^{7}$ &  --  & 207.51 &   \\ 
1--34 & 3p$^6$3d $^2$D$_{3/2}$--3p$^5$3d$^2$ $^4$D$_{1/2}$ & $8.9 \times 10^{-3}$ & $2.7 \times 10^{-3}$ & $2.0\times 10^{-3}$ & --  & $1.9\times 10^{8}$ &  --  & 214.21 &   \\ 
2--8 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^4$G$_{9/2}$ & $9.6 \times 10^{-3}$ & $1.1 \times 10^{-12}$ & 0.0 & --  & 0.82 &  --  & 245.12 &   \\ 
2--19 & 3p$^6$3d $^2$D$_{5/2}$--3p$^5$3d$^2$ $^2$F$_{5/2}$ & $8.9\times  10^{-3}$ & $5.5 \times 10^{-3}$ & $6.0\times 10^{-3}$ & --  & $1.1\times 10^{8}$ & 232.876 & 233.10 &    RR80 \\ 
 \hline                               
 \end{tabular}}
\par
\smallskip
\par
Notes: {the relative intensities  (photons)  ${\rm Int}=N_{j} A_{ji}/N_{\rm e}$ are normalised to 
the strongest transition and were calculated at an electron density of 10$^{9}$~cm$^{-3}$
and log $T$[K]~=~5.6.
Weighted  oscillator strengths $gf$ and \mbox{A-values} (s$^{-1}$) are from  the benchmark calculation.
The $gf$ values from G00 and the Z03 (case~D) calculation are also listed.
 $\lambda_{\rm exp}$ are our experimental wavelengths, while 
$\lambda_{\rm th}$  are the theoretical ones from the G00~energies.
The last column (ID) provides a key to previous identifications.
 N indicates a new one proposed here.} 
 \end{table}